The Use of Geometric Diversity for Spectral Dominance in Underground Imaging
|
|
- Jason McCarthy
- 5 years ago
- Views:
Transcription
1 The Use of Geoeic ivesiy fo pecal oiace i Udegoud Iagig Loezo Lo Moe, Rashid Asai, ailo icolo epae of lecical ad Copue gieeig Uivesiy of Illiois a Chicago Chicago, IL 667 looe@ece.uic.edu Michael C. Wics esos iecoae Ai Foce Reseach Laboaoy Roe, NY Michael.wics@l.af.il Absac Udegoud iagig of dielecic ad coducive aoalies pefoed usig goud peeaig adas (GPRs equies expesive widebad syses o icease he esoluio. The adve of oogaphic piciples i uli-oosaic GPRs daaically ipoved he iagig capabiliies ad suggesed he possibiliy of educig he badwidh of he pobig wavefo. I his wo we popose o exed he oogaphic piciples o he case of below-goud disibued sesig, hus aig advaage of he geoeic divesiy. We show ha, by usig geoeic divesiy, he fequecy coe equied o iage below-goud ages is dasically educed o viually a sigle oochoaic sigal, hus achievig full specal doiace i he wavefo desig. I. INTROUCTION Pesely, a pevale appoach o deec, locae, ace ad iage udegoud objecs is by usig Goud Peeaig Rada []-[5]. eph of peeaio is augeed by loggig daa hough boeholes. Iage esoluio is aelioaed by usig oogaphic piciples applied o he eceived daa [6]- [8]. Howeve, all GPR syses eed o use sho pulses (i.e. high fequecy badwidh o icease he ifoaio coceig he ages via fequecy divesiy. The use of high badwidh leads o seveal issues. Fis, he sigal o oise aio (NR deceases wih a icease i he specal coe of he pobig wavefield. ecod, he elecoageic specu available fo iliay ad civil applicaios is coiuously beig eoded due o he eedous dead of wieless applicaios. Fuheoe, uieioal (e.g. boadcasig saios o ieioal (e.g. jaes a-ade iefeeces ca educe he available specu. If lage badwidh is equied, MI, MC ad ieodulaio effecs becoe difficul ass o be acled ad solved. Thid, a widebad syse ca be exeely buly, delicae ad expesive. This poble is acceuaed whe he syse is desiged o wo a lowe fequecies: i is ipacical o geeae well-desiged sho pulses i he HF fequecy age, whee aeas ae fudaeally elecically sall. Addiioally, he shoe he pulse is, he geae is he difficuly ad cos i popely saplig he eceived sigal. Fouh, he coduciviy ad dielecic peiiviy of he goud vaies wih he fequecy: if a widebad sigal is se io he goud, fequecy dispesio is liely o occu, hus boadeig he pulse suppo ad educig he achievable esoluio. Addiioal o-badwidh elaed facos lii he efficiecy of coo GPRs. Fo exaple, he esoluio i aziuh depeds o he beawidh: a HF fequecies i is ipacical o ceae pecil beas, heefoe aziuh esoluio us be educed by usig ohe echiques. Moeove, coo GPR suffe fo he blid egio effec i which he eceive is idle uil he asie coplees he asissio of he pulse. This poble ca be solved by ivoig suiable odulaio echiques, a he pealy of iceased coplexiy ad cos of he syse. Fially, whe a age is o paallel o he suface, ule s law suggess ha efleced eegy is o aily bac-popagaig o he GPR eceive, ad hus is deecio ay be copoised. We popose a ehodology [9]-[4], aed RF oogaphy, ha addesses hese ope issues, ad we deosae how RF oogaphy ay oupefo cue sae-of-he-a GPR echology. RF oogaphy equies a se of low-cos peeable aspodes abiaily deployed above he goud (see Fig.. Tasies sed a wavefo io he goud, scaees e-iadiae powe owad eceives, which log daa ad elay he eieved ifoaio o a base saio. The ovely of his appoach is he use of uliple asies (i.e. view divesiy ad uliple eceives (i.e. obsevaio divesiy, besides fequecy, polaizaio ad aea pae divesiy. The accual of geoeic divesiy faciliaes he wavefo fequecy coe educio, ad i he liiig case a se of discee oochoaic sigals yield acioable below-goud 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
2 ecosuced iages. I his wo we focus o he ivesio algoihs ecessay o pocess he sigals easued by he uliude of goud sesos. = ω μ εε + jμ σ / ω = ω μ ε. (3 The fucio i ( accous fo he diffeece bewee he uow dielecic peiiviy of he objec ad ha of he hos ediu. Fo each poi holds: ' i egio, he veco wave equaio ( ' ε ( ' ( ' = +. (4 Figue : RF Toogaphy. Tasies sed powe io he goud. Receives collec he scaeed field ad sed his ifoaio o he ai saio. II. FORWAR MOL We descibe he fowad odel of a RF oogaphic syse by cosideig he 3 geoey depiced i Fig.. The hos ediu (i.e. he eah is odeled as a hoogeeous ediu wih elaive dielecic peiiviy ε, coduciviy σ, ad ageic peeabiliy μ. The ages ae assued o eside i he ivesigaio doai. The souces ae N elecically sall dipoles (of legh Δ l o loops (of aea A fed wih cue I, ad locaed a posiio (view divesiy. Fo each asiig aea, he scaeed field is colleced by M eceives (obsevaio divesiy, locaed a pois i space. Fo sipliciy, a sigle opeaig fequecy f is adoped. We assue he elaive dielecic peiiviy pofile ε ( ' ad he coduciviy pofile ( ' σ iside he ivesigaio doai as uows of he poble. Accodigly, he ivese poble is ecas i es of he uow peiiviy coas fucio: ( ' σ σ ε ( ' = ε( ' ε + j. ( π f ε I his way, he wave ube iside ca be expessed as: ( ' = ωμεε ( ' + jωμσ ( ' = + ε ( ', ( The scaeed wave i a poi ha is soluio of (4 ca be wie i es of iegal equaio of he dyadic Gee s fucio: ( = ( ( ( G, ' ' ' d ', (5 whee ( ' is he oal field i he ivesigaio doai, I give as he supeposiio of he icide field ( ' (i.e. he field i he ivesigaed aea whe objecs ae abse ad he field (, scaeed by he ages. As i is well ow, he ivese scaeig poble i (5 is o-liea. Neveheless, i ca be ecas o a liea poble by eas of he Bo appoxiaio (BA. Ude BA, he oal field iside he iegad of (5 ca be appoxiaed by he ow icide field [5]-[8], i.e.: ε I ( ( ( ( G, ' ' ' d '. (6 Theefoe, he ivese poble a had is cas as he ivesio of he liea iegal equaio coecig he peiiviy coas fucio o he scaeed field daa. The use of BA ca be jusified by cosideig ha: The ages of iees ae isolaed, liied i ube ad ebedded i a lossy ediu. Theefoe, uual ieacio (a pheoeo igoed by BA bewee ages ca be assued egligible. I geeal, he ihoogeeiies of he soil ae elecically sall, ad hei coduciviy eais low. Theefoe, hei scaeed fields ae isigifica copaed wih he RF sigal e-iadiaed by ou ages of iees. Ou goal is o deec, localize ad appoxiaely deeie he geoey of he ages. Towad his objecive i has bee show how BA based ivesio algoihs ae able o wo wih sog scaeig objecs, povided ha o quaiaive descipio of he dielecic peiiviy i is equied. ε 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
3 The Gee s fucio depeds upo he geoey ha is cosideed (half-space, wo-diesioal, full space. I his wo, we uilize he hee diesioal dyadic Gee s fucio G fo a hoogeeous ediu wih he sae popeies of he eah. This assupio is easoable because he sesos ae deployed a he ai/goud ieface, ad he fequecies ivolved ae elaively low. Accodigly, we have [9]: (, ' G j ' e = I + 4 π '. (7 The opeao i (7, which is esposible fo depolaizaio ad is useful fo ea field sesig, ca be geeally egleced fo ' >>, i.e. whe sesos ae locaed i he fa zoe wih espec o ages. The icide field, i.e. he field adiaed i he hoogeeous ediu fo a poi souce locaed a posiio, is give by: ( ', = Q ( ', ˆ G a, (8 I = ωμ Δ fo a elecically sall dipole, o whee Q j l I Q = jωμa I fo a elecically sall loop, a ˆ is he (elecic o ageic dipole oe diecio. Addiioally, he field eceived by a dipole o loop wih oe diecio ˆ a posiioed a due o a equivale (i es of I cue disibuio defied iside he ivesigaio doai ca be expessed as [8]: (, = I ( ( ε ( aˆ G, ' ', ' d '. (9 ubsiuig (8 i (9 we obai he scala fowad odel of RF oogaphy: (, = L( ε ( ' = Q ( ( ε ( a G, ' G ', a ' d '. ( Fo a aheaical poi of view, he poble of fidig he coas fucio is o pefo he ivese of he liea opeao L coecig he uow coas fucio ad he scaeed field daa. Figue : 3 Geoey fo he ivesio odel. III. INVRION PROCUR A. Tihoov Regulaizaio A way o copue L is o pefo a ueical ivesio of L []. Le us collec he sapled field daa i a odeed { } NM veco (, =, ad disceize he doai egio i K voxels, each oe locaed a posiio : he coas dielecic peiiviy ca be ebodied i a colu { } veco ε ε ( ' = of legh K, ad i epeses he se of uow paaees. Afe his disceizaio, eq. ( ca be ewie i a aix fo: = L ε, ( whee L ow is a aix wih diesios NM K. The poble is he o ive he elaio (. ue o he idepede se of easuees, L is heoeically full a, bu is ofe seveely ill-codiioed. This leads o sevee aifacs i he ecosucio pocess, paiculaly exacebaed whe oise (heal, exeal, quaizaio o clue is ipigig he eceives. A coo way o quaify he behavio of L is by ispecio of is codiio ube κ. Fo he opeao L i 6 is quie coo o obai ypical values of κ above. A efficie ehod o pefo a ivese of a vey ill codiioed aix is by usig he Tihoov egulaizaio pocedue. I his way, he coas dielecic peiiviy ca be esiaed: ( H H ˆ = + ε LL βi L ( ' 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
4 H Whee L deoes he adjoi of L, ad β is he egulaizaio paaee i he Tihoov sese, ha eeds o be appopiaely seleced. The advaage of his appoach is is eaable pefoace i geeaig eaigful iages, eve whe he ube of sesos is liied. Ufouaely, a pope choice of β ay be a difficul as, ad ofe i is ecessay o see fo a cosaied opiizaio soluio of β befoe a eaigful, shap ad low blued iage is ecosuced. This iplies a (copuaioally expesive aix ivesio fo each aep ay be ecessay. B. Fouie Appoach I pacical sceaios, whee eal-ie pocessig is ciical, o whe he elay o a base-saio is ipeded, i is pivoal o deive a ivesio saegy ha pivileges speed vs. accuacy. This pioiy is ephasized by he cue syse echology, which is widely ipleeig FFT ouies o acceleae iage ecosucios. Theefoe, we popose a appoach ha aes advaage of he Fouie elaio aisig bewee scaeed field ad objec shape, as discussed i lieaue ude he opic of diffacio oogaphy. I fac, if ages ad sesos ae disa eough so ha he popagaig wave is TM (oally occuig whe he fields ae piaily popagaig as /, he he fowad odel ca be expessed as follows below. We defie he ui o diecio of popagaio vecos as: ˆ l ˆsi cos ˆsi si ˆ = x θ ϕ y θ ϕ z cosθ, (3 ˆ l = xˆsiθ cosϕ + yˆsiθ siϕ + z ˆcosθ. (4 Usig he paaxial appoxiaio, he asiig Gee s fucio a he geeic posiio ' iside egio ca be siplified as: G (, ' ( ( ˆ + j + jl exp exp ', (5 4π while he eceivig Gee s fucio ca be expessed as: G ( ', ( ( ˆ + j jl exp exp '. (6 4π Theefoe, fo a pai of asies ad eceives, he scaees field ca be ewie as: (, 6π ( aˆ aˆ + j + Qe ε ( ( ˆ ˆ + j 'exp l l ' d' q. (7 is a siplified ad coiuous vesio of (. The quaiy ( ˆ ˆ veco:.(7 l l ca be epeseed by a 3 ( ˆ ˆ = l l. (8 q. (7 ca be ewie as [33]: ( 6π ( aˆ aˆ + j + = Qe ε ( ( + j 'exp ' d' I is useful o coside a oalized vesio of (9: ˆ ˆ a a ( 6π j + ( = e Q ( ( j. (9 ( = ε 'exp + ' d' ( This esul ca be iepeed i he followig way: each colleced saple ( eus he value of he specal copoe of he coas fucio ( ' ε. Theoeically, if we have eough saples o fully populae he specal epeseaio of ( ' ( fucio ( ε, he discee fucio i he lii ca be appoxiaed as a coiuous, ad ( ca be iepeed as a 3 ivese Fouie asfo of he peiiviy coas fucio. Theefoe, we ca ecosuc a iage of he udegoud by diec Fouie asfo eq. (9, i.e.: ( ( ( ˆ ε ' exp j ' d, ( = K whee he doai of iegaio K is he suppo of. By ispecio of (8, we coclude ha whe he ( sesos copleely ecicle he age, K is a sphee of adius, eaig ha he available ifoaio of he 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
5 specal coe of ( ' ε is liied up o he specal copoe. Theefoe, he ecosuced iage of he coas fucio will be a low-pass fileed vesio of he ue iage. I he eal sceaio whee a fiie ube of sesos ae deployed, hee facos affec he esoluio (leadig o bluig ad aifacs: he ivalidiy of paaxial appoxiaio, he o-uifo saplig, he spase daa se, ad he aeuaio cosa. I his wo, we coside he aeuaio o be egligible, so ha he wave ube i ( eais a eal quaiy, ad FFT ca be applied. Paaxial appoxiaio holds whe he agle θ bewee he ay passig hough he oigi ad he ay ax iesecig he bouday of he egio is egligible. This agle ca be copued usig: θ ( ' ˆ ˆ j ( ' ' l l j ax = ax ax a j ' ˆ ˆ ˆ j l j + l j l j, ( whee j epeses ay asie o eceive. Blu educio is accoplished by segeig he egio io salle aalysis egios (whee θ ax eais sall wihi he subegio ad by cosideig a ivese poble (i.e. salle FFT fo each sub-egio. The, he esulig sub-iages ae cocaeaed o fo he fial iage. The o-uifo o uifo gid asfoaio ca be accoplished usig Ti-Liea iepolaio. Le us defie a uifo gid i he specal doai of he scaeed field (,,, whee: Nxyz,, Nxyz,,,, = Δxyz,,, + Δxyz,,,... Nxyz,,, Δxyz,, Fo he i-liea iepolaio, le us defie hee ievals i (3 he Fouie space: Δ, Δ, Δ. Le us coside a saple poi (,, i he uifo gid o be esiaed, ad a o-uifo saple poi = + + ha has bee easued: we ca defie a iepolaio weighig faco as follows: ( ( ( w = h u h v h w (4 whee: x y z h xyz,, ( a The oal weighig faco is: a a Δ = Δ W x, yz, xyz,, (5 ohewise N M = w (6 = = The esiaed value i (,, is heefoe: N M u v w w (,, ( = (7 W = = The ajo advaage of his echique is he iisic possibiliy of esiae issig saples whe we choose Δ x, yz, >Δxyz,,. I his way, he ecosuced iage shows fewe aifacs ad fewe oscillaios. A way o ecove ifoaio fo he issig saples o he spase daase ca be accoplished by usig he echique of Pojecio o Covex se (POC. The basic idea of POC is o popely weigh he available saples i a way ha he coespode poi spead fucio is iiized. The ideal poi spead fucio (PF ( ' ( jux' + vy ' + wz ' = Δ Δ Δ (8 PF e u + v + w coicides wih he ipulse espose of he RF oogaphy opical syse, i.e. has he shape of a 3 Bessel-sic fucio, ad i ca be copued ueically by usig a 3 FFT algoih so ha he PF is ow fo ay value of ' i he egio. Fo sipliciy, le us coside a equivale scaled poble i which,, ad Δ Δ Δ = Howeve, he acual PF geeaed by he available saples is: N N N ( ' = s s s s s= jux ( ' vy' wz' (9 PF p e + + whee he weighig facos p s ae ideically equal o uiy. I piciple, by popely weighig he elees i he icoplee suaio (9, i ay be possible ha he weighed acual PF is poiwise vey siila o he ideal PF: 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
6 ( ', ', ' PF ( x ', y ', z ' PF (3 I ode o achieve his esul we ivoe he Pojecio o Covex es ehod, which is based o successive appoxiaios of he acual PF uil a soppig cieio is e. I he fis ieaio, we esiae he poi spead fucio by iposig all weighs o be p =. The ex sep is o copae poiwise he copued PF wih he ideal PF (i he pace doai. Moe exacly, we ceae a suiable guad bad egio o he ideal PF. If he values of he acual PF ae fallig ouside he guad egio, we foce hese values o be iside he guad egio. Oce he coecios o he copued PF ae doe, we pefo a 3 IFFT. The Fouie asfo of he coeced acual PF is geeally a fucio ha has values fo ay,, pais. The ex sep is o se o zeo all pois i he Fouie doai ha epese ou issig saples. I his way, we ae ceaig a ew fucio defied oly whee acual saples ae locaed. We pefo a ew copuaio of PF usig he values peviously obaied, ad he POC ieaio coiues fo uil a soppig cieio is e, e.g. he copued PF lies copleely wihi he guad bad egio, o he -h ieaio of he copued PF does o ipove he appoxiaio of he ideal PF wih espec of he -h ieaio, i.e. he pocess salls. Whe POC eiaes, he coefficie p s of he las ieaio ae used fo copuig he o-uifo ivese Fouie asfo of he eceived elecic field, as follows: p s Figue 4: ecosuced iage usig Fouie, o POC Figue 5: ecosuced iage usig Fouie ad POC jux ( s ' + vy s ' + wz s ' ˆ ε ( ' = pse ( us, vs, ws (3 s= IV. IMULATION AN RULT We pefoed seveal siulaios usig he ehods descibed above. The geoey is depiced i Fig. 3, he pobig fequecy is 3MHz, ad esuls ae show i Figs. 4,5,6. Cosideaios ad fuhe exaples will be show a he ie of he cofeece. Figue 6: ecosuced iage usig Tihoov Figue 3: : Geoey fo he siulaio (op view. Tasies ae epeseed wih +, while eceives ae epeseed wih X. The wo blac lies epese he posiios of he uels. V. ACKNOWLGMNT The auhos ae haful o M. W. Baldygo, Ai Foce Reseach Laboaoy, fo sposoig ad fudig his eseach. We ae also gaeful o M. J. Pae,. M. Feaa, Ai Foce Reseach Laboaoy,. F. oldoviei, Cosiglio Nazioale Riceche, Ialy, Pof. M. Cheey, Resselae Polyechic Isiue, fo hei echical discussios. 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
7 RFRNC [] R.J. Lyle,.F Laie,.L. Lage ad.j. avis Usig Coss Boehole lecoageic Pobig o Locae High Coas Aoalies, Geophysics. Vol. 44, pp , 979. [] A.J evaey, Geophysical iffacio Toogaphy I Tas o Geosci. Reoe es. Vol. G-, No., pp. 3-3, Ja [3]. J. aiels, Goud Peeaig Radas, ecod diio. Isiuio of lecical giees, Lodo, UK, 4. [4] A.J. Wie, J.. Molyeux, J.. Nyquis, Goud Peeaig Rada Toogaphy: Algoihs ad Case udies, I Tas. Geosci. Reoe es., Vol 3, No., pp , Ma [5] A.J. Wie, ad. Log, hallow Applicaios of Geophysical iffacio Toogaphy. I Tasacios o Geosciece ad Reoe es., Vol. 4, No. 5, p , ep. 986 [6] T. B. Hase, ad P. M. Johase, Ivesio chee fo Goud Peeaig Rada ha Taes Io Accou he Plaa Ai-oil Ieface, I Tas. Geosci. Reoe es., Vol. 38, No., pp , Ja. [7] T. J. Cui ad W. C. Chew, iffacio Toogaphic Algoih fo he eecio of Thee-iesioal Objecs Buied i a Lossy Half- pace, I Tasacios o Aeas ad Popagaio. Vol. 5, No., pp. 4-49, Ja.. [8] P. Meice, Liea GPR Ivesio fo Lossy oil ad a Plaa Ai- oil Ieface, I Tas. Geosci. ad Reoe es., Vol 39, No., pp. 73-7, ec. [9] M. C. Wics, RF Toogaphy wih Applicaio o Goud Peeaig Radas, I Poc. 4 s Asiloa Cofeece ACC 7, pp. 7-, 4-7 Nov. 7 [] L. Lo Moe,. icolo, ad M. C. Wics, Popagaio Model, Opial Geoey ad Receive esig fo RF Geooogaphy, I Poc. RadaCo 8, Roe, Ialy, May 6-3, 8. [] L. Lo Moe, A. M. Bagci,. icolo, ad R. Asai, paial Resoluio i Toogaphic Iagig wih iffaced Fields, Poc. XXIX Geeal Assebly of he Ieaioal Uio of Radio ciece (URI, Chicago, IL, UA, Aug. 7-6, 8. [] L. Lo Moe, ad. icolo, isibued RF Toogaphy fo Voids eecio, Poc. 8 Meeig fo he Miliay esig yposia (M, pecialy o Balespace Acousic ad eisic esig, Mageic ad lecic Field esos, Lauel, M, UA, Aug. 9-, 8. [3] J. Nogad, M.C. Wics, ad A. ozd, isibued/bedded ub- uface esos fo Iagig Buied Objecs wih Reduced Muual Couplig ad uppessed lecoageic issios, Poc. Ieaioal Cofeece o lecoageics i Advaced Applicaios (ICAA, pp , Tui, ep [4] L. Lo Moe, ad. icolo, Receivig Aea esig fo Goud Peeaig Toogaphic Iagig, Poc. I AP- Ieaioal yposiu, a iego, CA, UA, Jul. 5-, pp. -4, 8. [5] G. Leoe, F. oldoviei, Aalysis of he disoed Bo appoxiaio fo ubsuface Recosucio: Tucaio ad Uceaiiies ffec, I Tas. o Geosci. ad Reoe es., Vol. 4, No., pp , Ja. 3 [6] R. Pesico, R. Beii, F. oldoviei, The Role of he Measuee Cofiguaio i Ivese caeig fo Buied Objecs ude he Bo Appoxiaio, I Tas o Aeas Popag., Vol. 53, No. 6, pp , Ju 5 [7] H. J. Li ad F. L. Li, A Geealized Iepeaio ad Pedicio i Micowave Iagig Ivolvig Fequecy ad Agula ivesiy, J. lecoageic Waves ad Applicaios, Vol. 4, No. 5, pp , 99 [8] F. oldoviei, J. Hugeschid, R. Pesico, G. Leoe, A Liea Ivese caeig Algoih fo Realisic GPR Applicaios, Nea uface Geophysics, Vol. 5, No., pp. 9-4, Feb. 7 [9] W.C. Chew, Waves ad Fields i Ihoogeeous Media. I Pess, 995, Piscaaway NJ [] M. Beeo, ad P. Boccacci, Ioducio o Ivese Pobles i Iagig, Isiue of Physics Ld, Lodo, UK,. 9 Ieaioal W& Cofeece /9/$5. 9 I Auhoized licesed use liied o: WAHINGTON UNIVRITY LIBRARI. owloaded o Ocobe 6, 9 a 5:6 fo I Xploe. Resicios apply.
Parameter Optimization of Multi-element Synthetic Aperture Imaging Systems
Paaee Opiizaio of Muli-elee Syheic Apeue Iagig Syses Vea Beha Isiue fo Paallel Pocessig Bulgaia Acadey of Scieces 5-A Acad. G. Bochev S., Sofia 1113, Bulgaia E-ail: beha@bas.bg Received: Jauay 19, 7 Acceped:
More informationCameras and World Geometry
Caeas ad Wold Geoe How all is his woa? How high is he caea? Wha is he caea oaio w. wold? Which ball is close? Jaes Has Thigs o eebe Has Pihole caea odel ad caea (pojecio) ai Hoogeeous coodiaes allow pojecio
More informationSupplementary Information
Supplemeay Ifomaio No-ivasive, asie deemiaio of he coe empeaue of a hea-geeaig solid body Dea Ahoy, Daipaya Saka, Aku Jai * Mechaical ad Aeospace Egieeig Depame Uivesiy of Texas a Aligo, Aligo, TX, USA.
More informationSpectrum of The Direct Sum of Operators. 1. Introduction
Specu of The Diec Su of Opeaos by E.OTKUN ÇEVİK ad Z.I.ISMILOV Kaadeiz Techical Uivesiy, Faculy of Scieces, Depae of Maheaics 6080 Tabzo, TURKEY e-ail adess : zaeddi@yahoo.co bsac: I his wok, a coecio
More informationApplications of force vibration. Rotating unbalance Base excitation Vibration measurement devices
Applicaios of foce viaio Roaig ualace Base exciaio Viaio easuee devices Roaig ualace 1 Roaig ualace: Viaio caused y iegulaiies i he disiuio of he ass i he oaig copoe. Roaig ualace 0 FBD 1 FBD x x 0 e 0
More informationComparing Different Estimators for Parameters of Kumaraswamy Distribution
Compaig Diffee Esimaos fo Paamees of Kumaaswamy Disibuio ا.م.د نذير عباس ابراهيم الشمري جامعة النهرين/بغداد-العراق أ.م.د نشات جاسم محمد الجامعة التقنية الوسطى/بغداد- العراق Absac: This pape deals wih compaig
More informationOutline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem
adial diffsio eqaio Febay 4 9 Diffsio Eqaios i ylidical oodiaes ay aeo Mechaical Egieeig 5B Seia i Egieeig Aalysis Febay 4, 9 Olie eview las class Gadie ad covecio boday codiio Diffsio eqaio i adial coodiaes
More informationON POINTWISE APPROXIMATION OF FUNCTIONS BY SOME MATRIX MEANS OF FOURIER SERIES
M aheaical I equaliies & A pplicaios Volue 19, Nube 1 (216), 287 296 doi:1.7153/ia-19-21 ON POINTWISE APPROXIMATION OF FUNCTIONS BY SOME MATRIX MEANS OF FOURIER SERIES W. ŁENSKI AND B. SZAL (Couicaed by
More informationNumerical Solution of Sine-Gordon Equation by Reduced Differential Transform Method
Poceedigs of he Wold Cogess o Egieeig Vol I WCE, July 6-8,, Lodo, U.K. Nueical Soluio of Sie-Godo Equaio by Reduced Diffeeial Tasfo Mehod Yıldıay Kesi, İbahi Çağla ad Ayşe Beül Koç Absac Reduced diffeeial
More informationElectromagnetic Wave Absorber with Isotropic and Anisotropic Metamaterials
Ieaioal Joual of Maeials Sciece ad Applicaios 07; 6(6): 30-308 hp://www.sciecepublishiggoup.co/j/ijsa doi: 0.648/j.ijsa.070606.6 ISSN: 37-635 (Pi); ISSN: 37-643 (Olie) Elecoageic Wave Absobe wih Isoopic
More informationTransistor configurations: There are three main ways to place a FET/BJT in an architecture:
F3 Mo 0. Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils o povide biasig so ha he asiso has he coec
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationFBD of SDOF Base Excitation. 2.4 Base Excitation. Particular Solution (sine term) SDOF Base Excitation (cont) F=-(-)-(-)= 2ζω ωf
.4 Base Exiaio Ipoa lass of vibaio aalysis Peveig exiaios fo passig fo a vibaig base hough is ou io a suue Vibaio isolaio Vibaios i you a Saellie opeaio Dis dives, e. FBD of SDOF Base Exiaio x() y() Syse
More informationCapítulo. of Particles: Energy and Momentum Methods
Capíulo 5 Kieics of Paicles: Eegy ad Momeum Mehods Mecáica II Coes Ioducio Wok of a Foce Piciple of Wok & Eegy pplicaios of he Piciple of Wok & Eegy Powe ad Efficiecy Sample Poblem 3. Sample Poblem 3.
More informationINF 5460 Electronic noise Estimates and countermeasures. Lecture 13 (Mot 10) Amplifier Architectures
NF 5460 lecoic oise simaes ad couemeasues Lecue 3 (Mo 0) Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils
More informationABSOLUTE INDEXED SUMMABILITY FACTOR OF AN INFINITE SERIES USING QUASI-F-POWER INCREASING SEQUENCES
Available olie a h://sciog Egieeig Maheaics Lees 2 (23) No 56-66 ISSN 249-9337 ABSLUE INDEED SUMMABILIY FACR F AN INFINIE SERIES USING QUASI-F-WER INCREASING SEQUENCES SKAIKRAY * RKJAI 2 UKMISRA 3 NCSAH
More informationهقارنت طرائق تقذير هعلواث توزيع كاها ري املعلوتني
هقارنت طرائق تقذير هعلواث توزيع كاها ري املعلوتني يف حالت البياناث املفقودة باستخذام احملاكاة د أ. الباحثة ظافر حسين رشيد جامعة بغداد- كمية االدارة واالقتصاد قسم االحصاء آوات سردار وادي املستخلص Maxiu
More informationLow-Complexity Turbo Receiver for MIMO SC-FDMA Communication Systems
Poceedigs of he Wold Cogess o Egieeig 5 ol I WCE 5, Jly - 3, 5, Lodo,.K. Low-Coplexiy bo Receive fo IO SC-FDA Coicaio Syses Fag-Bia eg, Y-Ka Chag ad Yig- Yag Absac liple-ip liple-op (IO) echologies ae
More informationResearch Article On Pointwise Approximation of Conjugate Functions by Some Hump Matrix Means of Conjugate Fourier Series
Hidawi Publishig Copoaio Joual of Fucio Spaces Volue 5, Aicle ID 475, 9 pages hp://dx.doi.og/.55/5/475 Reseach Aicle O Poiwise Appoxiaio of Cojugae Fucios by Soe Hup Maix Meas of Cojugae Fouie Seies W.
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More informationOptical flow equation
Opical Flow Sall oio: ( ad ae le ha piel) H() I(++) Be foce o poible ppoe we ake he Talo eie epaio of I: (Sei) Opical flow eqaio Cobiig hee wo eqaio I he lii a ad go o eo hi becoe eac (Sei) Opical flow
More information6.2 Improving Our 3-D Graphics Pipeline
6.2. IMPROVING OUR 3-D GRAPHICS PIPELINE 8 6.2 Impovig Ou 3-D Gaphics Pipelie We iish ou basic 3D gaphics pipelie wih he implemeaio o pespecive. beoe we do his, we eview homogeeous coodiaes. 6.2. Homogeeous
More informationECSE Partial fraction expansion (m<n) 3 types of poles Simple Real poles Real Equal poles
ECSE- Lecue. Paial facio expasio (m
More informationRelations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems
Tish Joal of Aalysis ad Nmbe Theoy 27 Vol 5 No 4 26-3 Available olie a hp://pbssciepbcom/ja/5/4/2 Sciece ad Edcaio Pblishig DOI:269/ja-5-4-2 Relaios o he Aposol Type (p -Fobeis-Ele Polyomials ad Geealizaios
More informationSUSTAINABLE HEAT FARMING OF GEOTHERMAL SYSTEMS: A CASE STUDY OF HEAT EXTRACTION AND THERMAL RECOVERY IN A MODEL EGS FRACTURED RESERVOIR
PROCEEDINGS, Thiy-Sih Wokshop o Geoheal Resevoi Egieeig Safod Uivesiy, Safod, Califoia, Jauay 3 - Febuay, SGP-TR-9 SUSTAINABLE HEAT FARMING OF GEOTHERMAL SYSTEMS: A CASE STUDY OF HEAT EXTRACTION AND THERMAL
More informationThe Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues
Alied Maheaical Sciece Vol. 8 o. 5 747-75 The No-Tucaed Bul Aival Queue M x /M/ wih Reei Bali Sae-Deede ad a Addiioal Seve fo Loe Queue A. A. EL Shebiy aculy of Sciece Meofia Uiveiy Ey elhebiy@yahoo.co
More informationEfficient Interference Mitigation in mmwave Backhaul Network for High Data Rate 5G Wireless Communications
I. J. Couicaios Newok ad Syse Scieces 017 10 170-180 hp://www.scip.og/joual/ijcs ISSN Olie: 1913-373 ISSN Pi: 1913-3715 Efficie Iefeece Miigaio i Wave Backhaul Newok fo High Daa Rae 5G Wieless Couicaios
More informationM-ary Detection Problem. Lecture Notes 2: Detection Theory. Example 1: Additve White Gaussian Noise
Hi ue Hi ue -ay Deecio Pole Coide he ole of decidig which of hyohei i ue aed o oevig a ado vaiale (veco). he efoace cieia we coide i he aveage eo oailiy. ha i he oailiy of decidig ayhig ece hyohei H whe
More informationStatistical Optics and Free Electron Lasers
Saisical Opics ad Fee leco Lases ialuca eloi uopea XFL Los Ageles UCLA Jauay 5 h 07 Saisical Opics ad Fee leco Lases Theoy ialuca eloi UCLA Los Ageles Jauay 5 h 07 is difficul if o impossible o coceive
More informationEXACT ANALYSIS OF UNSTEADY CONVECTIVE DIFFUSION IN A HERSCHEL BULKLEY FLUID IN AN ANNULAR PIPE
Ieaioal Joual of Maheaics ad Copue Applicaios Reseach (IJMCAR) ISSN 49-6955 Vol. 3, Issue, Ma 3, 5-6 TJPRC Pv. Ld. EXACT ANALYSIS OF UNSTEADY CONVECTIVE DIFFUSION IN A HERSCHEL BULKLEY FLUID IN AN ANNULAR
More informationModel characterization of impulse response for diffuse optical indoor wireless channels
2005 WEA I. Cof. o DYNAMICAL YTEM ad CONTOL Veice Ialy Novembe 2-4 2005 pp545-550 Model caaceizaio of impulse espose fo diffuse opical idoo wieless caels Adia Miaescu Maius Oeseau Uivesiaea Polieica Timişoaa
More informationOn imploding cylindrical and spherical shock waves in a perfect gas
J. Fluid Mech. (2006), vol. 560, pp. 103 122. c 2006 Cambidge Uivesiy Pess doi:10.1017/s0022112006000590 Pied i he Uied Kigdom 103 O implodig cylidical ad spheical shock waves i a pefec gas By N. F. PONCHAUT,
More informationExistence and Smoothness of Solution of Navier-Stokes Equation on R 3
Ieaioal Joual of Mode Noliea Theoy ad Applicaio, 5, 4, 7-6 Published Olie Jue 5 i SciRes. hp://www.scip.og/joual/ijma hp://dx.doi.og/.436/ijma.5.48 Exisece ad Smoohess of Soluio of Navie-Sokes Equaio o
More informationPhysics 207 Lecture 13
Physics 07 Lecue 3 Physics 07, Lecue 3, Oc. 8 Agenda: Chape 9, finish, Chape 0 Sa Chape 9: Moenu and Collision Ipulse Cene of ass Chape 0: oaional Kineaics oaional Enegy Moens of Ineia Paallel axis heoe
More informationOne of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of
Oe of he commo descipios of cuilie moio uses ph ibles, which e mesuemes mde log he ge d oml o he ph of he picles. d e wo ohogol xes cosideed sepely fo eey is of moio. These coodies poide ul descipio fo
More informationSpectral Simulation of Turbulence. and Tracking of Small Particles
Specra Siuaio of Turbuece ad Trackig of Sa Parices Hoogeeous Turbuece Saisica ie average properies RMS veociy fucuaios dissipaio rae are idepede of posiio. Hoogeeous urbuece ca be odeed wih radoy sirred
More informationGENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS
GENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS HENDRA GUNAWAN Absac. Associaed o a fucio ρ :(, ) (, ), le T ρ be he opeao defied o a suiable fucio space by T ρ f(x) := f(y) dy, R
More informationTechnical Report: Bessel Filter Analysis
Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we
More informationON GENERALIZED FRACTIONAL INTEGRAL OPERATORS. ( ρ( x y ) T ρ f(x) := f(y) R x y n dy, R x y n ρ( y )(1 χ )
Scieiae Mahemaicae Japoicae Olie, Vol., 24), 37 38 37 ON GENERALIZED FRACTIONAL INTEGRAL OPERATORS ERIDANI, HENDRA GUNAWAN 2 AND EIICHI NAKAI 3 Received Augus 29, 23; evised Apil 7, 24 Absac. We pove he
More informationr r r r r EE334 Electromagnetic Theory I Todd Kaiser
334 lecoagneic Theoy I Todd Kaise Maxwell s quaions: Maxwell s equaions wee developed on expeienal evidence and have been found o goven all classical elecoagneic phenoena. They can be wien in diffeenial
More information1 Notes on Little s Law (l = λw)
Copyrigh c 26 by Karl Sigma Noes o Lile s Law (l λw) We cosider here a famous ad very useful law i queueig heory called Lile s Law, also kow as l λw, which assers ha he ime average umber of cusomers i
More informationRelation (12.1) states that if two points belong to the convex subset Ω then all the points on the connecting line also belong to Ω.
Lectue 6. Poectio Opeato Deiitio A.: Subset Ω R is cove i [ y Ω R ] λ + λ [ y = z Ω], λ,. Relatio. states that i two poits belog to the cove subset Ω the all the poits o the coectig lie also belog to Ω.
More informationThe Central Limit Theorems for Sums of Powers of Function of Independent Random Variables
ScieceAsia 8 () : 55-6 The Ceal Limi Theoems fo Sums of Poes of Fucio of Idepede Radom Vaiables K Laipapo a ad K Neammaee b a Depame of Mahemaics Walailak Uivesiy Nakho Si Thammaa 86 Thailad b Depame of
More informationTHE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN
THE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN Musafa KUTANIS Ad Muzaffe ELMAS 2 SUMMARY I is pape, a vaiaio of e FEM wic is so-called geeal subsucue meod is caied
More informationReal-time TDDFT simulations within SIESTA. Daniel Sánchez-Portal, Rafi Ullah, Fabiano Corsetti, Miguel Pruneda and Emilio Artacho
Real-ime TDDFT simulaios wihi SIESTA Daiel Sáchez-Poal, Rafi Ullah, Fabiao Cosei, Miguel Pueda ad Emilio Aacho Mai objecive Apply eal-ime simulaios wihi ime-depede desiy fucioal heoy TDDFT o sudy eleco
More informationNew Results on Oscillation of even Order Neutral Differential Equations with Deviating Arguments
Advace i Pue Maheaic 9-53 doi: 36/ap3 Pubihed Oie May (hp://wwwscirpog/oua/ap) New Reu o Ociaio of eve Ode Neua Diffeeia Equaio wih Deviaig Ague Abac Liahog Li Fawei Meg Schoo of Maheaica Sye Sciece aiha
More informationb : the two eigenvectors of the Grover iteration Quantum counting algorithm
.5.3. Quau couig algorih How quickly ca we deerie he uber of arge saes i Grover s algorih, i.e. arked saes, r, o a N= daa base search proble, if r is o kow i advace. Classical search ~ ( N ) Quau search
More informationFig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial
a b c Fig. S. The anenna consucion: (a) ain geoeical paaees, (b) he wie suppo pilla and (c) he console link beween wie and coaial pobe. Fig. S. The anenna coss-secion in he y-z plane. Accoding o [], he
More informationIdeal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory
Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable
More informationDuration Notes 1. To motivate this measure, observe that the duration may also be expressed as. a a T a
Duio Noes Mculy defied he duio of sse i 938. 2 Le he sem of pymes cosiuig he sse be,,..., d le /( + ) deoe he discou fco. he Mculy's defiiio of he duio of he sse is 3 2 D + 2 2 +... + 2 + + + + 2... o
More informationComparison between Fourier and Corrected Fourier Series Methods
Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1
More informationOn a Z-Transformation Approach to a Continuous-Time Markov Process with Nonfixed Transition Rates
Ge. Mah. Noes, Vol. 24, No. 2, Ocobe 24, pp. 85-96 ISSN 229-784; Copyigh ICSRS Publicaio, 24 www.i-css.og Available fee olie a hp://www.gema.i O a Z-Tasfomaio Appoach o a Coiuous-Time Maov Pocess wih Nofixed
More informationStrong Result for Level Crossings of Random Polynomials
IOSR Joual of haacy ad Biological Scieces (IOSR-JBS) e-issn:78-8, p-issn:19-7676 Volue 11, Issue Ve III (ay - Ju16), 1-18 wwwiosjoualsog Stog Result fo Level Cossigs of Rado olyoials 1 DKisha, AK asigh
More informationAvailable online at J. Math. Comput. Sci. 2 (2012), No. 4, ISSN:
Available olie a h://scik.og J. Mah. Comu. Sci. 2 (22), No. 4, 83-835 ISSN: 927-537 UNBIASED ESTIMATION IN BURR DISTRIBUTION YASHBIR SINGH * Deame of Saisics, School of Mahemaics, Saisics ad Comuaioal
More informationCAPACITY ANALYSIS OF ASYMPTOTICALLY LARGE MIMO CHANNELS. Georgy Levin
CAPACITY ANALYSIS OF ASYMPTOTICALLY LAGE MIMO CANNELS by Geogy Levi The hesis submied o he Faculy of Gaduae ad Posdocoal Sudies i paial fulfillme of he equiemes fo he degee of DOCTO OF PILOSOPY i Elecical
More informationS, we call the base curve and the director curve. The straight lines
Developable Ruled Sufaces wih Daboux Fame i iowsi -Space Sezai KIZILTUĞ, Ali ÇAKAK ahemaics Depame, Faculy of As ad Sciece, Ezica Uivesiy, Ezica, Tuey ahemaics Depame, Faculy of Sciece, Aau Uivesiy, Ezuum,
More informationUltrahigh Frequency Generation in GaAs-type. Two-Valley Semiconductors
Adv. Sudies Theo. Phys. Vol. 3 9 o. 8 93-98 lhigh Fequecy Geeio i GAs-ype Two-Vlley Seicoducos.. sov. K. Gsiov A. Z. Phov d A.. eiel Bu Se ivesiy 3 Z. Khlilov s. Az 48 Bu ciy- Physicl siue o he Azebij
More informationThe Importance of Ordering the Number of Lattice Points Inside a Rational Polyhedron Using Generating Functions
Ieraioal Joural of Copuer Sciece ad Elecroics Egieerig (IJCSEE Volue Issue ( ISSN 48 (Olie he Iporace of Orderig he Nuber of Laice ois Iside a Raioal olyhedro Usig Geeraig Fucios Halil Sopce Absrac I pure
More informationEXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar
Ieraioal Joural of Scieific ad Research Publicaios, Volue 2, Issue 7, July 22 ISSN 225-353 EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D S Palikar Depare of Maheaics, Vasarao Naik College, Naded
More informationPRESSURE BEHAVIOR OF HORIZONTAL WELLS IN DUAL-POROSITY, DUAL-PERMEABILITY NATURALLY-FRACTURED RESERVOIRS
VOL. NO. 8 MAY 5 ISSN 89-668 ARN Joual of Egieeig ad Applied Scieces 6-5 Asia Reseach ublishig Newok ARN. All ighs eseved. www.apjouals.co RESSURE BEHAVIOR OF HORIZONTAL WELLS IN UAL-OROSITY UAL-ERMEABILITY
More informationODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003
ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationBE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion
BE.43 Tuorial: Liear Operaor Theory ad Eigefucio Expasio (adaped fro Douglas Lauffeburger) 9//4 Moivaig proble I class, we ecouered parial differeial equaios describig rasie syses wih cheical diffusio.
More informationDavid Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.
! Revised April 21, 2010 1:27 P! 1 Fourier Series David Radall Assume ha u( x,) is real ad iegrable If he domai is periodic, wih period L, we ca express u( x,) exacly by a Fourier series expasio: ( ) =
More informationUNSTEADY HELICAL FLOWS OF A MAXWELL FLUID
PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY, Seies A, OF THE ROMANIAN ACADEMY Volue 5, Nube /4,. - UNSTEADY HELICAL FLOWS OF A MAXWELL FLUID Cosai FETECAU, Coia FETECAU Techical Uivesiy of Iasi,
More informationBorn-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna
Bo-Oppeheie Appoxiatio ad Noadiabatic Effects Has Lischa Uivesity of Viea Typical situatio. Fac-Codo excitatio fo the iiu of the goud state. Covetioal dyaics possibly M* ad TS 3. Coical itesectio fuel
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationNeutron Slowing Down Distances and Times in Hydrogenous Materials. Erin Boyd May 10, 2005
Neu Slwig Dw Disaces ad Times i Hydgeus Maeials i Byd May 0 005 Oulie Backgud / Lecue Maeial Neu Slwig Dw quai Flux behavi i hydgeus medium Femi eame f calculaig slwig dw disaces ad imes. Bief deivai f
More informationStrong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA
Iteatioal Joual of Reseach i Egieeig ad aageet Techology (IJRET) olue Issue July 5 Available at http://wwwijetco/ Stog Result fo Level Cossigs of Rado olyoials Dipty Rai Dhal D K isha Depatet of atheatics
More informationLESSON 15: COMPOUND INTEREST
High School: Expoeial Fuctios LESSON 15: COMPOUND INTEREST 1. You have see this fomula fo compoud ieest. Paamete P is the picipal amou (the moey you stat with). Paamete is the ieest ate pe yea expessed
More informationMultilevel-DFT based Low-Complexity Hybrid Precoding for Millimeter Wave MIMO Systems
Muieve-DFT based Low-Copexiy ybid Pecodig fo Miiee Wave MIMO yses Yu-si Liu, Chiag-e Che, Cheg-Rug Tsai, ad -Yeu (dy Wu, Feow, IEEE Gaduae Isiue of Eecoics Egieeig aioa Taiwa Uivesiy Taipei, Taiwa {ike,
More information[ m] x = 0.25cos 20 t sin 20 t m
. x.si ( 5 s [ ] CHAPER OSCILLAIONS x ax (.( ( 5 6. s s ( ( ( xax. 5.7 s s. x.si [] x. cos s Whe, x a x.5. s 5s.6 s x. x( x cos + si a f ( ( [ ] x.5cos +.59si. ( ( cos α β cosαcos β + siαsi β x Acos φ
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
More informationDegree of Approximation of Fourier Series
Ieaioal Mahemaical Foum Vol. 9 4 o. 9 49-47 HIARI Ld www.m-hiai.com h://d.doi.og/.988/im.4.49 Degee o Aoimaio o Fouie Seies by N E Meas B. P. Padhy U.. Misa Maheda Misa 3 ad Saosh uma Naya 4 Deame o Mahemaics
More informationThe Nehari Manifold for a Class of Elliptic Equations of P-laplacian Type. S. Khademloo and H. Mohammadnia. afrouzi
Wold Alied cieces Joal (8): 898-95 IN 88-495 IDOI Pblicaios = h x g x x = x N i W whee is a eal aamee is a boded domai wih smooh boday i R N 3 ad< < INTRODUCTION Whee s ha is s = I his ae we ove he exisece
More informationOn Acoustic Radiation by Rotating Dipole Sources in Frequency Domain
www.ccsee.org/as Moder Applied Sciece Vol. 5, No. 5; Ocober 211 O Acousic Radiaio by Roaig Dipole Sources i Frequecy Doai Zhihog Liu Ceer of Eergy ad Eviroe, QigDao Techological Uiversiy 11 FuShu Road,
More informationarxiv: v4 [math.pr] 20 Jul 2016
Submied o he Aals of Applied Pobabiliy ε-strong SIMULATION FOR MULTIDIMENSIONAL STOCHASTIC DIFFERENTIAL EQUATIONS VIA ROUGH PATH ANALYSIS axiv:1403.5722v4 [mah.pr] 20 Jul 2016 By Jose Blache, Xiyu Che
More informationBy the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences
Chapte : Theoy of Modula Aithmetic 8 Sectio D Chiese Remaide Theoem By the ed of this sectio you will be able to pove the Chiese Remaide Theoem apply this theoem to solve simultaeous liea cogueces The
More informationMathematical Models and the Soil Hydraulic Properties
Bullei UASVM Hoiculue 66/9 Pi ISSN 843-554; Elecoic ISSN 843-5394 Maeaical Model ad e Soil Hydaulic Popeie Floica MATEI Macel IRJA Ioaa POP Vioel BUIU Maia MICULA Faculy of Hoiculue Uiveiy of Agiculual
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More informationAnalysis of Stress in PD Front End Solenoids I. Terechkine
TD-05-039 Sepembe 0, 005 I. Ioducio. Aalysis of Sess i PD Fo Ed Soleoids I. Teechkie Thee ae fou diffee ypes of supecoducig soleoids used fo beam focusig i he Fod Ed of he Poo Dive. Table 1 gives a idea
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 4 9/16/2013. Applications of the large deviation technique
MASSACHUSETTS ISTITUTE OF TECHOLOGY 6.265/5.070J Fall 203 Lecure 4 9/6/203 Applicaios of he large deviaio echique Coe.. Isurace problem 2. Queueig problem 3. Buffer overflow probabiliy Safey capial for
More informationECE-314 Fall 2012 Review Questions
ECE-34 Fall 0 Review Quesios. A liear ime-ivaria sysem has he ipu-oupu characerisics show i he firs row of he diagram below. Deermie he oupu for he ipu show o he secod row of he diagram. Jusify your aswer.
More informationLow-complexity Algorithms for MIMO Multiplexing Systems
Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :
More informationChapter 31 Faraday s Law
Chapte 31 Faaday s Law Change oving --> cuent --> agnetic field (static cuent --> static agnetic field) The souce of agnetic fields is cuent. The souce of electic fields is chage (electic onopole). Altenating
More informationSolutions to selected problems from the midterm exam Math 222 Winter 2015
Soluios o seleced problems from he miderm eam Mah Wier 5. Derive he Maclauri series for he followig fucios. (cf. Pracice Problem 4 log( + (a L( d. Soluio: We have he Maclauri series log( + + 3 3 4 4 +...,
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationElectrical Engineering Department Network Lab.
Par:- Elecrical Egieerig Deparme Nework Lab. Deermiaio of differe parameers of -por eworks ad verificaio of heir ierrelaio ships. Objecive: - To deermie Y, ad ABD parameers of sigle ad cascaded wo Por
More informationTime Domain Modelling of Electromagnetic Field Propagation via Wave Potentials
BP: Compaioal lecomageics Time Domai Modellig o lecomageic ield Popagaio via Wave Poeials N. Geogieva Y. Rickad McMase Uivesi McMase Uivesi Depame o lecical ad Compe gieeig McMase Uivesi 8 Mai See Wes
More informationState-Space Model. In general, the dynamic equations of a lumped-parameter continuous system may be represented by
Sae-Space Model I geeral, he dyaic equaio of a luped-paraeer coiuou ye ay be repreeed by x & f x, u, y g x, u, ae equaio oupu equaio where f ad g are oliear vecor-valued fucio Uig a liearized echique,
More informationFARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09
FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this
More informationSecure Chaotic Spread Spectrum Systems
Seue Chaoi Sea Seum Sysems Ji Yu WSEAB ECE Deame Seves siue of Tehology Hoboke J 73 Oulie ouio Chaoi SS sigals Seuiy/ efomae ee eeives Biay oelaig eeio Mismah oblem aile-fileig base aoah Dual-aea aoah
More informationMultiparameter Golay 2-complementary sequences and transforms
Mulipaamee Golay -plemeay sequeces ad asfoms V.G. Labues, V.P. Chasovsih, E. Osheime Ual Sae Foes Egieeig Uivesiy, Sibisy a, 37, Eaeibug, Russia, 6000 Capica LLC, Pompao Beach, Floida, USA Absac. I his
More information1-D Sampling Using Nonuniform Samples and Bessel Functions
-D Saplig Usig Nouio Saples a Bessel Fuctios Nikolaos E. Myiis *, Mebe, IEEE,Electical Egiee, Ph.D. A & Chistooulos Chazas, Seio Mebe, IEEE, Poesso B A Cultual a Eucatioal Techologies Istitute, Tsiiski
More informationFARADAY'S LAW dt
FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,
More informationRobust Adaptive Control of Uncertain Nonlinear Systems in the Presence of Input Saturation and External Disturbance
67 IEEE RANSACIONS ON AUOMAIC CONROL, VOL. 56, NO. 7, JULY Robus Adapive Cool of Uceai Noliea Sysems i he Pesece of Ipu Sauaio ad Exeal Disubace Chagyu We, Fellow, IEEE, Jig Zhou, Membe, IEEE, Zhiao Liu,
More informationThe Alpha-Logarithmic Series Distribution of Order k and Some of Its Applications
oual of Saisical Theo ad Applicaios Vol. 5 No. 3 Sepembe 6 73-85 The Alpha-Logaihmic Seies Disibuio of Ode ad Some of Is Applicaios C. Saheesh Kuma Depame of Saisics Uivesi of Keala Tivadum - 695 58 Idia
More informationOn a Problem of Littlewood
Ž. JOURAL OF MATHEMATICAL AALYSIS AD APPLICATIOS 199, 403 408 1996 ARTICLE O. 0149 O a Poblem of Littlewood Host Alze Mosbache Stasse 10, 51545 Waldbol, Gemay Submitted by J. L. Bee Received May 19, 1995
More informationAdsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity
The Open-Access Jounal fo the Basic Pinciples of Diffusion Theoy, Expeient and Application Adsoption and Desoption Kinetics fo Diffusion Contolled Systes with a Stongly Concentation Dependent Diffusivity
More information